Spray pattern control with angular orientation in fuel injector and method

Information

  • Patent Grant
  • 6789754
  • Patent Number
    6,789,754
  • Date Filed
    Wednesday, September 25, 2002
    21 years ago
  • Date Issued
    Tuesday, September 14, 2004
    20 years ago
Abstract
Metering components of a fuel injector that allow spray targeting and distribution of fuel to be configured using non-angled or straight orifice having an axis parallel to a longitudinal axis of the fuel metering components. Metering orifices are located about the longitudinal axis and defining a first virtual circle greater than a second virtual or bolt circle defined by a projection of the sealing surface onto the metering disc so that all of the metering orifices are disposed outside the second virtual or bolt circle within one quadrant of the circle. A channel is formed between the seat orifice and the metering disc that allows the fuel injector to generate a spray pattern along the longitudinal axis that forms a flow area on a virtual plane transverse to the longitudinal axis. The fuel injector of the preferred embodiments can be calibrated to an angular position about the longitudinal axis to achieve a desired targeting of a flow area and desired flow area distribution and atomization of the fuel injector. A method of targeting the fuel flow area is also provided.
Description




BACKGROUND OF THE INVENTION




Most modern automotive fuel systems utilize fuel injectors to provide precise metering of fuel for introduction towards each combustion chamber. Additionally, the fuel injector atomizes the fuel during injection, breaking the fuel into a large number of very small particles, increasing the surface area of the fuel being injected, and allowing the oxidizer, typically ambient air, to more thoroughly mix with the fuel prior to combustion. The metering and atomization of the fuel reduces combustion emissions and increases the fuel efficiency of the engine. Thus, as a general rule, the greater the precision in metering and targeting of the fuel and the greater the atomization of the fuel, the lower the emissions with greater fuel efficiency.




An electromagnetic fuel injector typically utilizes a solenoid assembly to supply an actuating force to a fuel metering assembly. Typically, the fuel metering assembly is a plunger-style closure member which reciprocates between a closed position, where the closure member is seated in a seat to prevent fuel from escaping through a metering orifice into the combustion chamber, and an open position, where the closure member is lifted from the seat, allowing fuel to discharge through the metering orifice for introduction into the combustion chamber.




The fuel injector is typically mounted upstream of the intake valve in the intake manifold or proximate a cylinder head. As the intake valve opens on an intake port of the cylinder, fuel is sprayed towards the intake port. In one situation, it may be desirable to target the fuel spray at the intake valve head or stem while in another situation, it may be desirable to target the fuel spray at the intake port instead of at the intake valve. In both situations, the targeting of the fuel spray can be affected by the spray or cone pattern. Where the cone pattern has a large divergent cone shape, the fuel sprayed may impact on a surface of the intake port rather than towards its intended target. Conversely, where the cone pattern has a narrow divergence, the fuel may not atomize and may even recombine into a liquid stream. In either case, incomplete combustion may result, leading to an increase in undesirable exhaust emissions.




Complicating the requirements for targeting and spray pattern is cylinder head configuration, intake geometry and intake port specific to each engine's design. As a result, a fuel injector designed for a specified cone pattern and targeting of the fuel spray may work extremely well in one type of engine configuration but may present emissions and driveability issues upon installation in a different type of engine configuration. Additionally, as more and more vehicles are produced using various configurations of engines (for example: inline-4, inline-6, V-6, V-8, V-12, W-8 etc.,), emission standards have become stricter, leading to tighter metering, spray targeting and spray or cone pattern requirements of the fuel injector for each engine configuration.




It is believed that known metering orifices formed at an angle with respect to a longitudinal axis (i.e., “angled metering orifices”) of a fuel injector and arrayed in circular pattern along the longitudinal axis allow greater symmetry and greater latitude in configuring the fuel injector to operate with different engine configuration while achieving an acceptable level of fuel atomization, (quantifiable as an average Sauter-Mean-Diameter (SMD)). It is believed, however, that angled metering orifices require, at the present time, specialized machinery, trained operators and greater inefficiencies to manufacture than non-angled metering orifices. Moreover, even if the angled metering orifices can be competitively produced with the non-angled metering orifices, the angled metering orifices may still have uneven fuel distribution.




It would be beneficial to develop a fuel injector in which non-angled metering orifices can be used in controlling spray targeting and spray distribution of fuel. It would also be beneficial to develop a fuel injector in which increased atomization or precise targeting can be changed so as to meet a particular fuel targeting and cone pattern from one type of engine configuration to another type.




SUMMARY OF THE INVENTION




The present invention provides fuel targeting and fuel spray distribution at an acceptable level of fuel atomization with non-angled metering orifices. The present invention allows a fuel spray pattern of an injector to approximate a flow area downstream of the fuel injector so that regardless of a rotational orientation of the fuel injector about the longitudinal axis, the flow area can be achieved. In a preferred embodiment, a fuel injector is provided. The fuel injector includes a housing, a seat, a closure member and a metering disc. The housing has passageway extending between an inlet and an outlet along a longitudinal axis. The seat has a sealing surface facing the inlet and forming a seat orifice with a terminal seat surface spaced from the sealing surface and facing the outlet, and a first channel surface generally oblique to the longitudinal axis and is disposed between the seat orifice and the terminal seat surface. The closure member is disposed in the passageway and contiguous to the sealing surface so as to generally preclude fuel flow through the seat orifice in one position. The closure member is disposed in the passageway and contiguous to the sealing surface so as to generally preclude fuel flow through the seat orifice in one position. A magnetic actuator is disposed proximate the closure member so that, when energized, the actuator positions the closure member away from the sealing surface of the seat so as to allow fuel flow through the passageway and past the closure member. The metering disc is proximate to the seat and includes a second channel surface confronting the first channel surface so as to form a flow channel. The metering disc has at least two metering orifices located outside of the first virtual circle. The at least two metering orifices being located about the longitudinal axis at substantially equal arcuate distance apart between adjacent metering orifices. Each metering orifice extends generally parallel to the longitudinal axis between the second channel surface and a outer surface spaced from the second channel surface so that, when the magnetic actuator is energized to move the closure member, a flow of fuel through the metering orifices generates a spray pattern that intersects a virtual plane orthogonal to the longitudinal axis with a flow area having a plurality of different radii, one of the radii of the flow area including a maximum radius that, when rotated about the longitudinal axis, defines a circular area larger than a portion covered by the flow area such that targeting of the spray pattern requires orientation of the metering orifices about the longitudinal axis.




In yet another aspect of the present invention, a method of targeting a fuel flow area about a longitudinal axis is provided. The fuel injector includes a passageway extending between an inlet and outlet along a longitudinal axis, a seat and a metering disc. The seat has a sealing surface facing the inlet and forming a seat orifice. The seat has a terminal seat surface spaced from the sealing surface and facing the outlet, and a first channel surface generally oblique to the longitudinal axis and disposed between the seat orifice and the terminal seat surface. The closure member is disposed in the passageway and contiguous to the sealing surface so as to generally preclude fuel flow through the seat orifice in one position and disposed in another position spaced from the sealing surface to permit fuel flow through the passageway through the seat orifice. The metering disc has at least two metering orifices. Each metering orifice extends between second and outer surfaces along the longitudinal axis with the second surface facing the first channel surface. The method can be achieved, in part, by locating the at least two metering orifices outside of the first virtual circle, the metering orifices extending generally parallel to the longitudinal axis through the second and outer surfaces of the metering disc; flowing fuel through the at least two metering orifices upon actuation of the fuel injector so that a fuel flow path intersecting a virtual plane orthogonal to the longitudinal axis defines a flow area having a plurality of different radii about the longitudinal axis, one of the radii including a maximum radius that, when rotated about the longitudinal axis, defines a circular area larger than the flow area; and orientating the flow area about the longitudinal axis so as to adjust a targeting of the flow area towards a different portion of the circular area.











BRIEF DESCRIPTION OF THE DRAWINGS




The accompanying drawings, which are incorporated herein and constitute part of this specification, illustrate an embodiment of the invention, and, together with the general description given above and the detailed description given below, serve to explain the features of the invention.





FIG. 1

illustrates a preferred embodiment of the fuel injector.





FIG. 2A

illustrates a close-up cross-sectional view of an outlet end of the fuel injector of FIG.


1


.





FIG. 2B

illustrates a further close-up view of the preferred embodiment of the fuel metering components that, in particular, show the various relationships between various components in the subassembly.





FIG. 2C

illustrates two close-up views of two preferred embodiments of the fuel metering components that, in particular, show the various relationships between various components in the fuel metering components.





FIG. 2D

illustrates a generally linear relationship between spray cone size δ of fuel spray exiting the metering orifice to a radial velocity component of the fuel metering components.





FIG. 3

illustrates a perspective view of outlet end of the fuel injector of

FIG. 2A

that forms a flow area cross-section as the fuel spray intersects a virtual plane orthogonal to the longitudinal axis.





FIGS. 4A

,


4


B illustrates a preferred embodiment of the metering disc arranged on a bolt circle.





FIG. 5

illustrates a relationship between a ratio t/D of each metering orifice with respect to spray cone size for a specific configuration of the fuel injector.





FIGS. 6A

,


6


B, and


6


C illustrate the shape of the flow area approximates a circular area with increased number of metering orifices with attendant decrease in an cone size of the conical spray pattern.





FIGS. 7A and 7B

illustrate the fuel injector with a spray pattern generated during actuation of a preferred embodiment of the fuel injector.











DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS





FIGS. 1-7

illustrate the preferred embodiments. In particular, a fuel injector


100


having a preferred embodiment of the metering disc


10


is illustrated in FIG.


1


. The fuel injector


100


includes: a fuel inlet tube


110


, an adjustment tube


112


, a filter assembly


114


, a coil assembly


118


, a coil spring


116


, an armature


124


, a closure member


126


, a non-magnetic shell


110




a


, a first overmold


118


, a body


132


, a body shell


132




a


, a second overmold


119


, a coil assembly housing


121


, a guide member


127


for the closure member


126


, a seat


134


, and a metering disc


10


.




The guide member


127


, the seat


134


, and the metering disc


10


form a stack that is coupled at the outlet end of fuel injector


100


by a suitable coupling technique, such as, for example, crimping, welding, bonding or riveting. Armature


124


and the closure member


126


are joined together to form an armature/closure member assembly. It should be noted that one skilled in the art could form the assembly from a single component. Coil assembly


120


includes a plastic bobbin on which an electromagnetic coil


122


is wound.




Respective terminations of coil


122


connect to respective terminals


122




a


,


122




b


that are shaped and, in cooperation with a surround


118




a


formed as an integral part of overmold


118


, to form an electrical connector for connecting the fuel injector to an electronic control circuit (not shown) that operates the fuel injector.




Fuel inlet tube


110


can be ferromagnetic and includes a fuel inlet opening at the exposed upper end. Filter assembly


114


can be fitted proximate to the open upper end of adjustment tube


112


to filter any particulate material larger than a certain size from fuel entering through inlet opening before the fuel enters adjustment tube


112


.




In the calibrated fuel injector, adjustment tube


112


has been positioned axially to an axial location within fuel inlet tube


110


that compresses preload spring


116


to a desired bias force that urges the armature/closure member such that the rounded tip end of closure member


126


can be seated on seat


134


to close the central hole through the seat. Preferably, tubes


110


and


112


are crimped together to maintain their relative axial positioning after adjustment calibration has been performed.




After passing through adjustment tube


112


, fuel enters a volume that is cooperatively defined by confronting ends of inlet tube


110


and armature


124


and that contains preload spring


116


. Armature


124


includes a passageway


128


that communicates volume


125


with a passageway


113


in body


130


, and guide member


127


contains fuel passage holes


127




a


,


127




b


. This allows fuel to flow from volume


125


through passageways


113


,


128


to seat


134


.




Non-ferromagnetic shell


110




a


can be telescopically fitted on and joined to the lower end of inlet tube


110


, as by a hermetic laser weld. Shell


110




a


has a tubular neck that telescopes over a tubular neck at the lower end of fuel inlet tube


110


. Shell


110




a


also has a shoulder that extends radially outwardly from neck. Body shell


132




a


can be ferromagnetic and can be joined in fluid-tight manner to non-ferromagnetic shell


110




a


, preferably also by a hermetic laser weld.




The upper end of body


130


fits closely inside the lower end of body shell


132




a


and these two parts are joined together in fluid-tight manner, preferably by laser welding. Armature


124


can be guided by the inside wall of body


130


for axial reciprocation. Further axial guidance of the armature/closure member assembly can be provided by a central guide hole in member


127


through which closure member


126


passes.




Prior to a discussion of fuel metering components proximate the outlet end of the fuel injector


100


, it should be noted that the preferred embodiments of a seat and metering disc of the fuel injector


100


allow for a targeting of the fuel spray pattern (i.e., fuel spray separation) to be selected without relying on angled orifices. Moreover, the preferred embodiments allow the cone pattern (i.e., a narrow or large divergent cone spray pattern) to be selected based on the preferred spatial orientation of inner wall surfaces of the metering orifices being parallel to the longitudinal axis (i.e. so that the longitudinal axis of the wall surfaces is parallel to the longitudinal axis).




Referring to a close up illustration of the fuel metering components of the fuel injector in

FIG. 2A

which has a closure member


126


, seat


134


, and a metering disc


10


. The closure member


126


includes a spherical surface shaped member


126




a


disposed at one end distal to the armature. The spherical member


126




a


engages the seat


134


on seat surface


134




a


so as to form a generally line contact seal between the two members. The seat surface


134




a


tapers radially downward and inward toward the seat orifice


135


such that the surface


134




a


is oblique to the longitudinal axis A—A. The seal can be defined as a sealing circle


140


formed by contiguous engagement of the spherical member


126




a


with the seat surface


134




a


, shown here in

FIGS. 2A and 3

. The seat


134


includes a seat orifice


135


, which extends generally along the longitudinal axis A—A of the metering disc and is formed by a generally cylindrical wall


134




b


. Preferably, a center


135




a


of the seat orifice


135


is located generally on the longitudinal axis A—A. As used herein, the terms “upstream” and “downstream” denote that fuel flow generally in one direction from inlet through the outlet of the fuel injector while the terms “inward” and “outward” refer to directions toward and away from, respectively, the longitudinal axis A—A. And the longitudinal axis A—A is defined as the longitudinal axis of the metering disc, which in the preferred embodiments, is coincident with a longitudinal axis of the fuel injector.




Downstream of the circular wall


134




b


, the seat


134


tapers along a portion


134




c


towards a first metering disc surface


134




e


, which is spaced at a thickness “t” from a second metering disc surface or outer surface


134




f


. The taper of the portion


134




c


preferably can be linear or curvilinear with respect to the longitudinal axis A—A, such as, for example, a linear taper


134


(

FIG. 2B

) or a curvilinear taper


134




c


′ that forms an compound curved dome (FIG.


2


C).




In one preferred embodiment, the taper of the portion


134




c


is linearly tapered (

FIG. 2B

) in a downward and outward direction at a taper angle β away from the seat orifice


135


to a point radially past at least one metering orifice


142


. At this point, the seat


134


extends along and is preferably parallel to the longitudinal axis so as to preferably form cylindrical wall surface


134




d


. The wall surface


134




d


extends downward and subsequently extends in a generally radial direction to form a bottom surface


134




e


, which is preferably perpendicular to the longitudinal axis A—A. Alternatively, the portion


134




c


can extend through to the surface


134




e


of the seat


134


. Preferably, the taper angle β is about 10 degrees relative to a plane transverse to the longitudinal axis A—A. In another preferred embodiment, as shown in

FIG. 2C

, the taper is a second-order curvilinear taper


134




c


′ which is suitable for applications that may require tighter control on the constant velocity of fuel flow. Generally, however, the linear taper


134




c


is believed to be suitable for its intended purpose in the preferred embodiments.




The interior face


144


of the metering disc


10


proximate to the outer perimeter of the metering disc


10


engages the bottom surface


134




e


along a generally annular contact area. The seat orifice


135


is preferably located wholly within the perimeter, i.e., a “bolt circle”


150


defined by an imaginary line connecting a center of each of at least two metering orifices


142


symmetrical about the longitudinal axis. That is, a virtual extension of the surface of the seat


135


generates a virtual orifice circle


151


(

FIG. 4A

) preferably disposed within the bolt circle


150


of metering orifices disposed at equal arcuate distance between adjacent metering orifices.




The cross-sectional virtual extensions of the taper of the seat surface


134




b


converge upon the metering disc so as to generate a virtual circle


152


(FIGS.


2


B and


4


). Furthermore, the virtual extensions converge to an apex


139




a


located within the cross-section of the metering disc


10


. In one preferred embodiment, the virtual circle


152


of the seat surface


134




b


is located within the bolt circle


150


of the metering orifices. The bolt circle


150


is preferably entirely outside the virtual circle


152


. It is preferable that all of the metering orifices


142


are outside the virtual circle


152


such that an edge of each metering orifice can be on part of the boundary of the virtual circle but without being inside of the virtual circle. Preferably, the at least two metering orifices


142


include two to six metering orifices equally spaced about the longitudinal axis.




A generally annular controlled velocity channel


146


is formed between the seat orifice


135


of the seat


134


and interior face


144


of the metering disc


10


, illustrated here in FIG.


2


A. Specifically, the channel


146


is initially formed at an inner edge


138




a


between the preferably cylindrical surface


134




b


and the preferably linearly tapered surface


134




c


, which channel terminates at an outer edge


138




b


proximate the preferably cylindrical surface


134




d


and the terminal surface


134




e


. As viewed in

FIGS. 2B and 2C

, the channel changes in cross-sectional area as the channel extends outwardly from the inner edge


138




a


proximate the seat to the outer edge


138




b


outward of the at least one metering orifice


142


such that fuel flow is imparted with a radial velocity between the orifice and the at least one metering orifice.




That is to say, a physical representation of a particular relationship has been discovered that allows the controlled velocity channel


146


to provide a constant velocity to fluid flowing through the channel


146


. In this relationship, the channel


146


tapers outwardly from a first cylindrical area defined by the product of the pi-constant (π), a larger height hi with corresponding radial distance D


1


to a substantially equal second cylindrical area defined by the product of the pi-constant (π), a smaller height h


2


with correspondingly larger radial distance D


2


. Preferably, a product of the height h


1


, distance D


1


and it is approximately equal to the product of the height h


2


, distance D


2


and it (i.e. D


1


*h


1


*π=D


2


*h


2


*π or D


1


*h


1


=D


2


*h


2


) formed by a taper, which can be linear or curvilinear. The distance h


2


is believed to be related to the taper in that the greater the height h


2


, the greater the taper angle β is required and the smaller the height h


2


, the smaller the taper angle P is required. An annular space


148


, preferably cylindrical in shape with a length D


2


, is formed between the preferably linear wall surface


134




d


and an interior face of the metering disc


10


. And as shown in

FIGS. 2A and 3

, a frustum is formed by the controlled velocity channel


146


downstream of the seat orifice


135


, which frustum is contiguous to preferably a right-angled cylinder formed by the annular space


148


.




In another preferred embodiment, the cylinder of the annular space


148


is not used and instead a frustum forming part of the controlled velocity channel


146


is formed. That is, the channel surface


134




c


extends all the way to the surface


134




e


contiguous to the metering disc


10


, and referenced in

FIGS. 2B and 2C

as dashed lines. In this embodiment, the height h


2


can be referenced by extending the distance D


2


from the longitudinal axis A—A to a desired point transverse thereto and measuring the height h


2


between the metering disc


10


and the desired point of the distance D


2


. It is believed that the channel surface in this embodiment has a tendency to increase a sac volume of the seat, which may be undesirable in various fuel injector applications. Preferably the desired distance D


2


can be defined by an intersection of a transverse plane intersecting the channel surface


134




c


or


134




c


′ at a location at least 25 microns outward of the radially outermost perimeter of each metering orifice


142


.




By providing a constant velocity of fuel flowing through the controlled velocity channel


146


, it is believed that a sensitivity of the position of the at least two metering orifices


142


relative to the seat orifice or the longitudinal axis in spray targeting and spray distribution is minimized. That is to say, due to manufacturing tolerances, acceptable level concentricity of the array of metering orifices


142


relative to the seat orifice


135


or the longitudinal axis may be difficult to achieve. As such, features of the preferred embodiment are believed to provide a metering disc for a fuel injector that is believed to be less sensitive to concentricity variations between the array of metering orifices


142


on the bolt circle


150


and the seat orifice


135


. Further, it has been determined in a laboratory environment, as compared with known fuel injectors using non-angled orifices with the same operating parameters (e.g., fuel pressure, fuel type, ambient and fuel temperatures) but without configuration of the preferred embodiments, the fuel injectors of the preferred embodiment have achieved generally between 10 to 15 percent better atomization of fuel (via measurements of SauterMean-Diameter) for the fuel spray of the fuel injectors of the preferred embodiments. Moreover, the metering components can be manufactured using proven techniques such as, for example, punching, casting, stamping, coining and welding without resorting to specialized machinery, operators or techniques.




Further, it has been discovered that not only is the flow at a generally constant velocity through a preferred configuration of the controlled velocity channel


146


so as to diverge at a cone size δ as a function of the radial velocity component of the fuel flow (FIG.


2


D), it has been discovered that the flow through the metering orifices


142


tends to generate at least two vortices within the metering orifices. The at least two vortices generated in the metering orifice can be confirmed by modeling a preferred configuration of the fuel metering components via Computational-Fluid-Dynamics, which is believed to be representative of the true nature of fluid flow through the metering orifice. For example, as shown in

FIG. 4B

, flow lines flowing radially outward from the seat orifice


135


tend to be generally curved inwardly proximate the orifice


142




a


so as to form at least two vortices


143




a


and


143




b


within a perimeter of the metering orifice


142




a


, which is believed to enhance spray atomization of the fuel flow exiting each of the metering orifices


142


. Furthermore, as illustrated in

FIG. 3

, by providing at least two metering orifices, fuel flow through the metering disc forms a spray pattern


161


that intersects a virtual plane


162


orthogonal to the longitudinal axis A—A so as to form a flow area


164


. The flow area


164


has a plurality of unequal radii extending from the longitudinal axis such as, for example, R


1


, R


2


and R


3


(FIGS.


6


A-


6


C). The flow area


164


can also be generally symmetrical about the longitudinal axis A—A (

FIGS. 6A-C

and


7


A-


7


B).




By imparting a different radial velocity to fuel flowing through the seat orifice


135


, it has been discovered that a spray cone size δ resulting from a fuel flow through the at least two metering orifices (

FIG. 7A

) can be changed as a generally linear function of the radial velocity in FIG.


2


D. That is, an increase in a radial velocity component of the fuel flowing through the channel will result in an increase in a spray cone size δ, and a decrease in the radial velocity component of the fuel flow through channel will result in a decrease in the spray cone size δ. For example, in a preferred embodiment shown here in

FIG. 2D

, by changing a radial velocity component of the fuel flowing (between the orifice


135


and the at least two metering orifices


142


through the controlled velocity channel


146


) from approximately 8 meter-per-second to approximately 13 meter-per-second, the spray cone size δ changes correspondingly from approximately 13 degrees to approximately 26 degrees. The radial velocity can be changed preferably by changing the configuration of the fuel metering components (including D


1


, h


1


, D


2


or h


2


of the controlled velocity channel


146


), changing the flow rate of the fuel injector, or by a combination of both.




Furthermore, it has also been discovered that the cone size δ of the fuel spray is related to the aspect ratio t/D, where “t” is equal to a through length of the orifice and “D” is the largest diametrical distance between the inner surface of the orifice. The ratio t/D can be varied from 0.3 to 1.0 or greater. As the aspect ratio increases or decreases, the cone size δ becomes narrower or wider correspondingly. Where the distance D is held constant, the larger the thickness “t”, the narrower the cone size δ. Conversely, where the thickness “t” is smaller with the distance D held constant, the cone size δ is wider. In particular, the cone size δ is linearly and inversely related to the aspect ratio t/D, shown here in

FIG. 5

of a preferred embodiment. Here, as the ratio changes from approximately 0.3 to approximately 0.7, the cone size δ generally changes linearly and inversely from approximately 22 degrees to approximately 8 degrees. Hence, it is believed that cone size δ can be accomplished by configuring either the velocity channel


146


and space


148


, as discussed earlier or the aspect ratio t/D while the symmetry of the flow area


164


can be configured by the number of metering orifices equally spaced about the longitudinal axis. Although the through-length “t” (i.e., the length of the metering orifice along the longitudinal axis A—A) is shown in

FIG. 2B

as being substantially the same as that of the thickness of the metering disc


10


, it is noted that the thickness of the metering disc can be different from the through-length “t” of the metering orifice


142


.




The metering disc


10


has at least two metering orifices


142


. Each metering orifice


142


has a center located generally on an imaginary “bolt circle”


150


shown here in FIG.


4


. For clarity, each metering orifice is labeled as


142




a


,


142




b


,


142




c


. . . and so on in

FIGS. 3 and 4A

. Although each metering orifice


142


is preferably circular so that the distance D is generally the same as the diameter of the circular orifice (i.e., between diametrical inner surfaces of the circular opening), other orifice configurations, such as, for examples, square, rectangular, arcuate or slots can also be used. The metering orifices


142


are arrayed in a preferably circular configuration, which configuration, in one preferred embodiment, can be generally concentric with the virtual circle


152


. A seat orifice virtual circle


151


(

FIG. 4A

) is formed by a virtual projection of the orifice


135


onto the metering disc such that the seat orifice virtual circle


151


is outside of the virtual circle


152


and preferably generally concentric to both the first and second virtual or bolt circle


150


. The preferred configuration of the metering orifices


142


and the channel allows a flow path “F” of fuel extending radially from the orifice


135


of the seat in any one radial direction away from the longitudinal axis towards the metering disc passes to one metering orifice.




In addition to spray targeting with adjustment of the radial velocity and cone size δ determination by the controlled velocity channel and the aspect ratio t/D, respectively, a spatial orientation of the non-angled orifice openings


142


can also be used to shape the pattern of the fuel spray by changing the arcuate distance “L” between the metering orifices


142


along a bolt circle


150


in another preferred embodiment.

FIGS. 6A-6C

illustrate the effect of arraying the metering orifices


142


on progressively smaller equal arcuate distances between adjacent metering orifices


142


so as to increase a circularity of the flow area


164


with corresponding decreases in the cone size δ. This effect can be seen starting with metering disc


10


and moving through metering discs


10




a


and


10




b.






In

FIG. 6A

, relatively large equal arcuate distances L


1


between the metering orifices relative to each other form a wide cone pattern. The cone pattern of the fuel spray intersects a virtual plane (orthogonal to the longitudinal axis) to define a generally symmetrical flow area about the longitudinal axis. The generally symmetrical flow area has a plurality of radii R


1


, R


2


, R


3


and so on extending from the longitudinal axis that are generally not equal to each other. In

FIG. 6B

, spacing the metering orifices


142


at a smaller equal arcuate distance L


2


than the arcuate distances L


1


in

FIG. 6A

forms a relatively narrower cone pattern. In

FIG. 6C

, spacing the metering orifices


142


at even smaller equal arcuate distances L


3


between each metering orifice


142


forms an even narrower cone pattern. Furthermore, as can be seen in

FIGS. 6A-6C

, the circularity of the respective flow areas increases toward that of a circle. It should also be noted that a arcuate distance can be a linear distance between closest inner wall surfaces or edges of respective adjacent metering orifices on the bolt circle


151


. Preferably, the linear distance is greater than or equal to the thickness “t” of the metering disc.




The adjustment of arcuate distances can also be used in conjunction with the process previously described so as to tailor the spray geometry of a fuel injector to a specific engine design using non-angled metering orifices (i.e. openings having a generally straight bore generally parallel to the longitudinal axis A—A) while permitting the fuel injector of the preferred embodiments to be insensitive to its angular orientation about the longitudinal axis.




The targeting of the fuel injector can also be performed by angular adjustment of the metering disc


10


relative to the longitudinal axis or by angular adjustment of the housing of the fuel injector relative to the longitudinal axis so as to achieve a desired targeting configuration. In particular, a test injector of the preferred embodiments can be tested with a specific engine configuration by flowing fuel through the at least two metering orifices so that a fuel flow out of the injector intersects a virtual plane orthogonal to the longitudinal axis and defines a flow area with a plurality of different radii about the longitudinal axis. One of the radii (R


1


, R


2


, R


3


. . . ) defining the flow area includes a maximum radius R


max


that, when rotated about the longitudinal axis, defines an imaginary circular area


170


larger than a portion covered by the flow area of fuel (e.g., fuel flow area such as


164


,


166


or


168


). The imaginary circular area


170


has uncovered portions


163


which are not impinged by fuel flow on the virtual plane spaced at distance P. Where the portion covered by the flow area is not a desired target portion, the flow area can be oriented about the longitudinal axis so as to adjust a targeting of the flow area towards a different portion of the imaginary circular area


170


such as the non-covered portions


163


. That is, where targeting of the flow area requires orientation of the metering orifices about the longitudinal axis, either the metering disc or the fuel injector can be oriented. In particular, to reorient the flow area on a different angular portion of the imaginary circular area


170


, the metering disc can be rotated angularly about the longitudinal axis and then fixed to the body or the seat so as to form a hermetic seal by a suitable technique such as, for example, hermetic laser weld, lap welding or bonding. Alternatively, the metering disc can be angularly fixed relative to a reference point on the body of the fuel injector. Upon installation into a fuel rail or manifold, the housing of the fuel injector can be rotated about the longitudinal axis to another reference point on the fuel rail or fuel injector cup and then locked into position, thereby providing a desired targeting of the fuel flow area for the particular engine configuration. Subsequently, fuel injectors for this particular engine configuration can be orientated at the desired targeting configuration by one or a combination of the preceding procedures. And by re-orientating the flow area as needed for a specific engine configuration, as described above, a desired fuel spray targeting towards a specific portion of area with the imaginary circular area


170


defined by the maximum radius R


max


can be achieved.




In operation, the fuel injector


100


is initially at the non-injecting or unactuated position shown in FIG.


1


. In this position, a working gap exists between the annular end face


110




b


of fuel inlet tube


110


and the confronting annular end face


124




a


of armature


124


. Coil housing


121


and tube


12


are in contact at


74


and constitute a stator structure that is associated with coil assembly


18


. Non-ferromagnetic shell


110




a


assures that when electromagnetic coil


122


is energized, the magnetic flux will follow a path that includes armature


124


. Starting at the lower axial end of housing


34


, where it is joined with body shell


132




a


by a hermetic laser weld, the magnetic circuit extends through body shell


132




a


, body


130


and eyelet to armature


124


, and from armature


124


across working gap


72


to inlet tube


110


, and back to housing


121


.




When electromagnetic coil


122


is energized, the spring force on armature


124


can be overcome and the armature is attracted toward inlet tube


110


, reducing working gap


72


. This unseats closure member


126


from seat


134


open the fuel injector so that pressurized fuel in the body


132


flows through the seat orifice and through orifices formed on the metering disc


10


. It should be noted here that the actuator may be mounted such that a portion of the actuator can disposed in the fuel injector and a portion can be disposed outside the fuel injector. When the coil ceases to be energized, preload spring


116


pushes the closure member closed on seat


134


.




As described, the preferred embodiments, including the techniques or method of generating a spray pattern, are not limited to the fuel injector described but can be used in conjunction with other fuel injectors such as, for example, the fuel injector sets forth in U.S. Pat. No. 5,494,225 issued on Feb. 27, 1996, or the modular fuel injectors set forth in Published U.S. Patent Application No. 2002/0047054A1, published on Apr. 25, 2002, which is pending, and wherein both of these documents are hereby incorporated by reference in their entireties.




While the present invention has been disclosed with reference to certain embodiments, numerous modifications, alterations and changes to the described embodiments are possible without departing from the sphere and scope of the present invention, as defined in the appended claims. Accordingly, it is intended that the present invention not be limited to the described embodiments, but that it has the full scope defined by the language of the following claims, and equivalents thereof.



Claims
  • 1. A fuel injector comprising:a housing having a passageway extending between an inlet and an outlet along a longitudinal axis; a seat having a sealing surface facing the inlet and forming a seat orifice, a terminal seat surface spaced from the sealing surface and facing the outlet, a first channel surface generally oblique to the longitudinal axis and disposed between the seat orifice and the terminal seat surface; a closure member disposed in the passageway and contiguous to the sealing surface so as to generally preclude fuel flow through the seat orifice in one position and away from the sealing surface of the seat so as to allow fuel flow through the passageway past the closure member in another position; a magnetic actuator proximate the closure member that positions the closure member away from the sealing surface of the seat when energized so as to allow fuel flow through the passageway and past the closure member; and a metering disc proximate the seat so that a virtual projection of the sealing surface onto the metering disc defines a first virtual circle about the longitudinal axis, the metering disc including a second channel surface confronting the first channel surface so as to form a flow channel, the metering disc having at least two metering orifices being located about the longitudinal axis at substantially equal arcuate distance apart between adjacent metering orifices outside the first virtual circle, each of the metering orifices extending generally parallel to the longitudinal axis between the second channel surface and an outer surface of the metering disc so that, when the magnetic actuator is energized to move the closure member, a flow of fuel through the metering orifices generates a spray pattern that intersects a virtual plane orthogonal to the longitudinal axis with a flow area having a plurality of different radii, one of the radii of the flow area including a maximum radius that, when rotated about the longitudinal axis, defines a circular area larger than a portion covered by the flow area, such that targeting of the spray pattern requires orientation of the metering orifices about the longitudinal axis.
  • 2. The fuel injector of claim 1, wherein the metering disc comprises the outer surface being spaced from the second channel surface of the metering disc at a first thickness of at least 50 microns, and a first arcuate spacing comprises a linear distance between closest edges of adjacent metering orifices at least equal to approximately the first thickness.
  • 3. The fuel injector of claim 2, wherein the first thickness of the metering disc comprises a thickness selected from a group comprising one of approximately 75, 100, 150, and 200 microns.
  • 4. The fuel injector of claim 2, wherein the first thickness of the metering disc comprises a thickness of approximately 125 microns.
  • 5. The fuel injector of claim 1, wherein the at least two metering orifices comprise an aspect ratio of between approximately 0.3 and 1.0, the aspect ratio being generally equal to approximately a length of each of the metering orifice between the second channel and outer surfaces of the metering disc divided by approximately the largest distance perpendicular to the longitudinal axis between any two diametrical inner surfaces of each of the metering orifices.
  • 6. The fuel injector of claim 5, wherein the aspect ratio is inversely and generally related in a linear manner to an included angle between distal outer boundaries of the spray pattern.
  • 7. The fuel injector of claim 1, wherein first channel surface comprises an inner edge being located at approximately a first distance from the longitudinal axis and at approximately a first spacing along the longitudinal axis relative to the metering disc and an outer edge being located at approximately a second distance from the longitudinal axis and at approximately a second spacing from the metering disc along the longitudinal axis, such that a product of the first distance and first spacing is generally equal to a product of the second distance and second spacing.
  • 8. The fuel injector of claim 1, wherein the projection of the sealing surface further converging at a virtual apex disposed within the metering disc, and the flow channel comprises a second portion extending from the first portion, the second portion having a constant sectional area as the flow channel extends along the longitudinal axis.
  • 9. The fuel injector of claim 8, wherein the second distance is located at an intersection of a plane transverse to the longitudinal axis and the channel surface such that the intersection is at least 25 microns radially outward of the perimeter of a metering orifice.
  • 10. The fuel injector of claim 1, wherein the flow area is located at least 50 millimeters from an outer surface of the metering disc along the longitudinal axis.
  • 11. The fuel injector of claim 1, wherein the first portion of the flow channel comprises a generally frustoconical channel having a taper of about ten degrees with respect to a plane transverse to the longitudinal axis.
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